Abstract

In this study, we estimated source process of the 2016 Kumamoto earthquake from strong-motion data by using the multiple-time window linear kinematic waveform inversion method to discuss generation of strong motions and to explain crustal deformation pattern with a seismic source inversion model. A four-segment fault model was assumed based on the aftershock distribution, active fault traces, and interferometric synthetic aperture radar data. Three western segments were set to be northwest-dipping planes, and the most eastern segment under the Aso caldera was examined to be a southeast-dipping plane. The velocity structure models used in this study were estimated by using waveform modeling of moderate earthquakes that occurred in the source region. We applied a two-step approach of the inversions of 20 strong-motion datasets observed by K-NET and KiK-net by using band-pass-filtered strong-motion data at 0.05–0.5 Hz and then at 0.05–1.0 Hz. The rupture area of the fault plane was determined by applying the criterion of Somerville et al. (Seismol Res Lett 70:59–80, 1999) to the inverted slip distribution. From the first-step inversion, the fault length was trimmed from 52 to 44 km, whereas the fault width was kept at 18 km. The trimmed rupture area was not changed in the second-step inversion. The source model obtained from the two-step approach indicated 4.7 × 1019 Nm of the total moment release and 1.8 m average slip of the entire fault with a rupture area of 792 km2. Large slip areas were estimated in the seismogenic zone and in the shallow part corresponding to the surface rupture that occurred during the Mj7.3 mainshock. The areas of the high peak moment rate correlated roughly with those of large slip; however, the moment rate functions near the Earth surface have low peak, bell shape, and long duration. These subfaults with long-duration moment release are expected to cause weak short-period ground motions. We confirmed that the southeast dipping of the most eastern segment is more plausible rather than northwest-dipping from the observed subsidence around the central cones of the Aso volcano.Graphical .

Highlights

  • The 2016 Kumamoto earthquake, with Japan Meteorological Agency (JMA) magnitude (Mj) of 7.3, occurred at 01:25 JST on April 16, 2016, following the Mj6.5 earthquake occurring at 21:26 on 14 April

  • The source region of the 2016 Kumamoto earthquake is located on the Beppu–Shimabara graben system, which is situated in the central part of Kyushu Island

  • We examined the four-segment model with a southeast-dipping F1 segment because subsidence of the vertical deformation around the central cones of the Aso volcano observed by interferometric synthetic aperture radar (InSAR) and global navigation satellite system (GNSS) data suggests that the segment dips in that direction

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Summary

Introduction

The 2016 Kumamoto earthquake, with Japan Meteorological Agency (JMA) magnitude (Mj) of 7.3, occurred at 01:25 JST on April 16, 2016, following the Mj6.5 earthquake occurring at 21:26 on 14 April. In order to examine the appropriateness of the inverted velocity structure model, we simulated the waveforms of the S1 (Mw3.9) and S3 (Mw4.2) earthquakes (Fig. 1) assuming a point source with a rise time of 0.7 s. Estimation of source process We applied a two-step approach of the multi-time window linear waveform inversions of strong-motion data (Hartzell and Heaton 1983) to estimate the rupture process for the fault model. For this inversion analysis, seven smoothed ramp functions were assumed for each subfault.

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